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<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong> <strong>and</strong> <strong>motivation</strong><br />

Aleš Janka<br />

office Math <strong>0.</strong>107<br />

ales.janka@unifr.ch<br />

http://perso.unifr.ch/ales.janka/<strong>mechanics</strong><br />

September 22, 2010, Université de Fribourg<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>What</strong> <strong>is</strong> <strong>Continuum</strong> <strong>mechanics</strong>?<br />

<strong>0.</strong> <strong>Introduction</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> = domain of physics <strong>and</strong> engineering describing:<br />

elasticity <strong>and</strong> plasticity of solids <strong>and</strong><br />

dynamics of fluids (liquids or gases).<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>What</strong> <strong>is</strong> a continuum?<br />

A continuum = a physical object with mass which can be mapped<br />

onto points of a subdomain Ω ⊂ IR 3 . Mass d<strong>is</strong>tribution in Ω <strong>is</strong><br />

supposed to be continuous:<br />

for any subdomain ω ⊂ Ω, the mass m ω of ω <strong>is</strong> calculated by<br />

∫<br />

m ω = dm<br />

<strong>and</strong> small changes in the size of ω produce small changes in m ω .<br />

ω<br />

<strong>What</strong> <strong>is</strong> a continuum?<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

Modeling objects as continua neglects atomic, molecular <strong>and</strong><br />

crystal structure of mass.<br />

The continuum approach <strong>is</strong> nevertheless a good approximation on<br />

length scales much greater than the molecular scale.<br />

<strong>What</strong> does continuum <strong>mechanics</strong> do?<br />

Applies fundamental physical laws (conservation of mass,<br />

momentum <strong>and</strong> energy, force equilibrium . . . ) to continua to<br />

derive differential equations describing their behavior.<br />

Information about the particular material of the continua <strong>is</strong> added<br />

through an empiric constitutive relation / law.<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in engineering: crash-tests<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in engineering: crash-tests<br />

<strong>0.</strong> <strong>Introduction</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in engineering: crash-tests<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in engineering: aeronautics<br />

<strong>0.</strong> <strong>Introduction</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in engineering: aeronautics<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. weather forecasts<br />

<strong>0.</strong> <strong>Introduction</strong><br />

Meteosu<strong>is</strong>se forecast for Sep 22, 2010, temperatures<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in natural sciences: formation of galaxies (fluid dynamics)<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in natural sciences: formation of galaxies (fluid dynamics)<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in medicine (bone <strong>and</strong> t<strong>is</strong>sue <strong>mechanics</strong>, blood flow)<br />

from Arbenz, van Lenthe, Mennel, Müller <strong>and</strong> Sala: A scalable multi-level<br />

preconditioner for matrix-free µ-finite element analys<strong>is</strong> of human bone<br />

structures, Int. J. Numer. Meth. in Engineering 73 (2008), pp. 927–947<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in medicine (bone <strong>and</strong> t<strong>is</strong>sue <strong>mechanics</strong>, blood flow)<br />

from Arbenz, van Lenthe, Mennel, Müller <strong>and</strong> Sala: A scalable multi-level<br />

preconditioner for matrix-free µ-finite element analys<strong>is</strong> of human bone<br />

structures, Int. J. Numer. Meth. in Engineering 73 (2008), pp. 927–947<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


<strong>Continuum</strong> <strong>mechanics</strong> in practice<br />

.. in biology (t<strong>is</strong>sue <strong>mechanics</strong> <strong>and</strong> growth)<br />

from Schmundt et al. 2006<br />

Programme<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

Kinematic description of a continuum: deformation <strong>and</strong><br />

motion of Ω.<br />

Mechanical equilibria <strong>and</strong> conservation laws.<br />

Constitutive laws of materials: elastic <strong>and</strong> v<strong>is</strong>co-elastic<br />

materials, Newtonian fluids.<br />

Typical problems of continuum <strong>mechanics</strong>: analytical <strong>and</strong><br />

numerical solution of elasto-statics/dynamics, compressible<br />

<strong>and</strong> incompressible elasticity, Newtonian fluids.<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


Necessary mathematical techniques<br />

Mechanical state <strong>and</strong> properties of a continuum are<br />

independent of the choice of a coordinate system.<br />

We will introduce <strong>and</strong> use tensor calculus: covariant <strong>and</strong><br />

contravariant tensors <strong>and</strong> basic tensor operations, tensor fields in<br />

euclidean space, derivatives of tensors.<br />

Solutions of differential equations will be calculated analytically<br />

(on simple problems) or numerically: we will (re)-introduce the<br />

basics of a finite element method.<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

The beauty of simple analytical formulas: rubber baloon<br />

Great deal of underst<strong>and</strong>ing through a simple toy model<br />

Inflate a rubber party-balloon with an internal gas pressure p<br />

Initially, the baloon stretches to two different diameters, why?<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


The beauty of simple analytical formulas: rubber baloon<br />

Great deal of underst<strong>and</strong>ing through a simple toy model<br />

Force equilibrium on the cut:<br />

σ<br />

t<br />

r<br />

r0<br />

r<br />

p<br />

|F σ | = |F p |<br />

2πrtσ = πr 2 p<br />

elastic stress: σ = Eε = 2πr − 2πr 0<br />

2πr 0<br />

E<br />

rubber incompressibility: 4πr 2 t = 4πr 2 0 t 0<br />

p(r) = 2E t 0 r 2 0<br />

r 3 r − r 0<br />

r 0<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

The beauty of simple analytical formulas: rubber baloon<br />

Great deal of underst<strong>and</strong>ing through a simple toy model<br />

Force equilibrium on the cut:<br />

|F σ | = |F p |<br />

2πrtσ = πr 2 p<br />

elastic stress: σ = Eε = 2πr − 2πr 0<br />

2πr 0<br />

rubber incompressibility: 4πr 2 t = 4πr 2 0 t 0<br />

p(r) = 2E t 0 r 2 0<br />

r 3 r − r 0<br />

r 0<br />

E<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


The beauty of mathematical analys<strong>is</strong>: singularities<br />

Why it breaks always at a kink?<br />

von Mieses stress: indicator of plastic deformation <strong>and</strong> rupture<br />

Mathematical analys<strong>is</strong> of the solution of elasticity equations<br />

predicts, that rupture occurs in re-entrant corners (kinks)!<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

The beauty of mathematical analys<strong>is</strong>: (in)stability<br />

Buckling phenomenon<br />

The nightmare of civil engineers <strong>and</strong> architects<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


The beauty of mathematical analys<strong>is</strong>: (in)stability<br />

Buckling phenomenon<br />

The nightmare of civil engineers <strong>and</strong> architects<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong><br />

The beauty of mathematical analys<strong>is</strong>: (in)stability<br />

Buckling phenomenon<br />

The nightmare of civil engineers <strong>and</strong> architects<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>


The beauty of mathematical analys<strong>is</strong>: (in)stability<br />

Buckling phenomenon<br />

But it can also be exploited to our advantage!<br />

shock absorber for road safety<br />

<strong>Continuum</strong> <strong>mechanics</strong><br />

<strong>0.</strong> <strong>Introduction</strong>

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